The electromagnetic field carries both linear and angular momentum which can be exchanged during the field-matter interaction, and yield a radiation pressure and radiation torque on the matter [1]}.
In the past few  decades, the field of light-matter interaction has grown impressively after the invention of optical tweezers [2]} that have played an indispensable role with countless applications [3]}, [4]}. In optical tweezers setups, the trapping and manipulating of spherical objects are obtained near to the focus point of a tightly focused continuous-wave laser beam [5]}, [6]}, [7]}, [8]}, while the long-range optical manipulation of chiral and dielectric objects can be achieved by using a structured Bessel beam or two non-collinear plane waves [9]}, [10]}, [11]}, [12]}, [13]}, [14]}.
